Content-aware resizing of uniform rosette color halftone images

ABSTRACT

As provided herein, there are supplied teachings to systems and methods for resizing a digital uniform rosette halftone image composed of multiple colorant separations, by using uniform rosette halftone tile parameters. One approach entails receiving into a digital imaging system, a digital uniform rosette halftone image and a desired resizing factor for that digital uniform rosette halftone image. Subsequently the system will define uniform rosette cells within the color uniform rosette digital halftone image. From the defined uniform rosette cells, a number of uniform rosette halftone tile seams are determined for manipulation. The orientation of the number of uniform rosette halftone tile seams is dictated by the received desired resizing factor. An energy map of the digital uniform rosette halftone image is determined according to an energy metric derived from the multiple colorant separations. The energy of the number of uniform rosette halftone tile seams within the energy map is determined so as to provide indication of at least one low energy determined uniform rosette halftone tile seam. A resizing of the uniform rosette halftone image by manipulating the at least one low energy determined uniform rosette halftone tile seam is performed so as to obtain a resized uniform rosette halftone image. The resized uniform rosette halftone image may then be printed on a printer.

CROSS-REFERENCE TO COPENDING APPLICATIONS

Attention is directed to copending applications filed concurrentlyherewith: U.S. application Ser. No. ______, Attorney Docket No.20071591-US-NP, entitled “Content-Aware Halftone Image Resizing”; U.S.application Ser. No. ______, Attorney Docket No. 20071591Q-US-NP,entitled “Content-Aware Halftone Image Resizing Using IterativeDetermination of Energy Metrics”; and U.S. application Ser. No. ______,Attorney Docket No. 20080380Q-US-NP, entitled “Content-Aware UniformRosette Color Halftone Image Resizing Using Iterative Determination ofEnergy Metrics”; the disclosure found in these copending applications ishereby incorporated by reference in their entirety. The appropriatecomponents and processes of the above co-pending applications may beselected for the teaching and support of the present application inembodiments thereof.

BACKGROUND AND SUMMARY

The teachings herein are directed to a method and apparatus for resizinga color halftone image using uniform rosette halftone tile parameters.

Demands imposed by today's digital media handling in regards to documentedit-ability, portability, and dynamic layout make simple solutions forimage resizing obsolete. Consider that a document can be rasterized andhalftoned for a particular print path. That document may be directed toa different printer, possibly years later when extracted from anarchive, with different paper size capabilities and may require imageediting, cropping and resizing of halftoned image content prior toprinting on the given print engine. Color halftone images may generallybe re-purposed to print on different paper sizes and require layoutmodifications and resizing. Printed color halftone images may be scannedin a setting such as at a digital copier, and a user may wish to modifythe image attributes such as size, aspect ratio, or image content.Conventional resizing methods that utilize spatially consistentinterpolation methods are unsuitable in this halftone image settingbecause interpolation methods introduce defects in color halftone imagestructure and such spatially consistent interpolation can distort imagecontent.

To begin, consider the halftone image class of concern to the presentteachings herein. With the advent of inexpensive digital color printers,methods and systems of color digital halftoning have become increasinglyimportant in the reproduction of printed or displayed images possessingcontinuous color tones. It is well understood that most digital colorprinters operate in a binary mode, i.e., for each color separation, acorresponding color spot is either printed or not printed at a specifiedlocation or pixel. Digital halftoning controls the printing of colorspots, where the spatial averaging of the printed color spots by eithera human visual system or a viewing instrument, provides the illusion ofthe required continuous color tones.

The most common halftone technique is screening, which compares therequired continuous color tone level of each pixel for each colorseparation with one or more predetermined threshold levels. Thepredetermined threshold levels are typically defined for a rectangularcell that is tiled to fill the plane of an image, thereby forming ahalftone screen of threshold values. At a given pixel, if the requiredcolor tone level is darker than the given halftone threshold level, acolor spot is printed at that specified pixel. Otherwise the color spotis not printed. The output of the screening process is a binary patternof multiple small “dots,” which are regularly spaced as is determined bythe size, shape, and tiling of the halftone cell. In other words, thescreening output, as a two-dimensionally repeated pattern, possesses twofundamental spatial frequencies, which are completely defined by thegeometry of the halftone screen.

It is understood in the art that the distribution of printed pixelsdepends on the design of the halftone screen. For clustered-dot halftonescreens, all printed pixels formed using a single halftone celltypically group into one or more clusters. If a halftone cell onlygenerates a single cluster, it is referred to as a single-dot halftoneor single-dot halftone screen. Alternatively, halftone screens may bedual-dot, tri-dot, quad-dot, or the like.

While halftoning is often described in terms of halftone dots, it shouldbe appreciated that idealized halftone dots can possess a variety ofshapes that include rectangles, squares, lines, circles, ellipses, “plussigns,” X-shapes, pinwheels, and pincushions, and actual printed dotscan possess distortions and fragmentation of those idealized shapesintroduced by digitization and the physical printing process. Variousdigital halftone screens having different shapes and angles aredescribed in U.S. Pat. No. 4,149,194, the disclosure found therein ishereby incorporated by reference in its entirety.

A common problem that arises in digital color halftoning is themanifestation of moiré patterns. Moiré patterns are undesirableinterference patterns that occur when two or more color halftoneseparations are printed over each other. Since color mixing during theprinting process is a non-linear process, frequency components otherthan the fundamental frequencies and harmonics of the individual colorhalftone separations can occur in the final printout. For example, if anidentical halftone screen is used for two color separations,theoretically, there should be no moiré patterns. However, any slightmisalignment between the two color halftone separations occurring froman angular difference and/or a scalar difference will result in twoslightly different fundamental frequency vectors. Due to nonlinear colormixing the difference in frequency vectors produces a beat frequencywhich will be visibly evident as a very pronounced moiré interferencepattern in the output. To avoid, for example, two-color moiré patternsdue to misalignment, or for other reasons, different halftone screensare commonly used for different color separations, where the fundamentalfrequency vectors of the different halftone screens are separated byrelatively large angles. Therefore, the frequency difference between anytwo fundamental frequencies of the different screens will be largeenough so that no visibly objectionable moiré patterns are produced.

In selecting different halftone screens, for example for three colorseparations, it is desirable to avoid any two-color moiré as well as anythree-color moiré. It is well known that in the traditional printingindustry that three halftone screens, which can be constructed byhalftone cells that are square in shape and identical, can be placed at15°, 45°, and 75°, respectively, from a point and axis of origin, toprovide the classical three-color moiré-free solution.

However, for digital halftoning, the freedom to rotate a halftone screenis limited by the raster structure, which defines the position of eachpixel. Since tan(15°) and tan(75°) are irrational numbers, rotating ahalftone screen to 15° or 75° cannot be exactly implemented in digitalhalftoning. To this end, some methods have been proposed to provideapproximate instead of exact moiré-free solutions. For example, in U.S.Pat. Nos. 5,323,245 and 5,583,660, this problem is approached by using acombination of two or more perpendicular, unequal frequency screenpatterns and non-perpendicular, equal frequency non-conventional screenpatterns. However, all these approximate solutions result in somehalftone dots having centers that do not lie directly on addressablepoints, or on the pixel positions defined by the raster structure.Therefore, the shape and center location varies from one halftone dot toanother. Consequently, additional interference or moiré between thescreen frequencies and the raster frequency can occur. In anotherapproach, U.S. Pat. No. 5,371,612 discloses a moiré prevention method todetermine screen angles and sizes that is usable solely forsquare-shaped, halftone screens.

U.S. Pat. No. 6,798,539 to Wang et al., discloses methods for usingsingle-cell, non-orthogonal clustered-dot screens to satisfy themoiré-free conditions for color halftoning. The disclosure also providesmethods that combine single-cell non-orthogonal clustered-dot screensand line screens for moiré-free color halftoning. Particularly, theselection of these single-cell halftone screens is determined bysatisfying moiré-free conditions provided in the respective spatial orfrequency equations. The disclosure found in U.S. Pat. No. 6,798,539 ishereby incorporated by reference in its entirety.

In U.S. Patent Application Publication No. 2006/0170975 A1, Wangdiscloses a moiré-free color halftone configuration for clustered dots.Unlike conventional methods, the disclosed method produces periodichexagon rosettes of identical shapes. These exemplary hexagon rosetteshave three fundamental spatial frequencies exactly equal to half of thefundamental frequency of the three halftone screens. The resultanthalftone outputs are truly moiré free, as all the fundamentals andharmonic frequencies are multiples of and thus higher in frequency thanthe rosette fundamental frequency. The disclosure found in U.S. PatentApplication Publication No. 2006/0170975 A1 is hereby incorporated byreference in its entirety

In U.S. Patent Application Publication No. 2008/0130055 A1, Wang andLoce disclose a method and apparatus for moiré-free color halftoneprinting with up to four color image separations. The method andapparatus utilize a plurality of non-orthogonal halftone screens toproduce outputs that are moiré free and form uniform periodic rosettes.The method and apparatus provide for defining a first and a second colorhalftone screen fundamental frequency vector for each of three halftonescreens such that the halftone screen set output forms uniform hexagonalrosettes; then defining a fourth color halftone screen where a firstfundamental vector of the fourth screen shares a fundamental frequencyvector with one of said three halftone screens and a second fundamentalfrequency vector of the fourth screen shares a fundamental frequencyvector with a different one of said three color halftone screens. Thedisclosure found in U.S. Patent Application Publication No. 2008/0130055is hereby incorporated by reference in its entirety.

In U.S. Patent Application Publication No. 2008/0130054, Wang and Locedisclose a method and apparatus for moiré-free enhanced color halftoneprinting of color image separations for an arbitrary number ofcolorants. The method and apparatus utilizes a plurality of halftonescreens, >4, to produce outputs that are moiré free and form hexagonalperiodic rosettes. The relatively large number of screens can be usedfor enhanced printing applications, such as printing with high-fidelitycolorants, light colorants, or special colorants, such as white,metallics and fluorescents. The method and apparatus provide fordefining rosette fundamental frequency vectors V_(R1), V_(R2) thatsatisfy a length and sum requirement to meet visual acceptabilitystandards according to |V_(R1)|>f_(min), |V_(R2)|>f_(min), and|V_(R1)±V_(R2)|>f_(min); defining N halftone screens for colorants i=1,N, respectively possessing first and second frequency vectors (V_(i1),V_(i2)), where no two screens possess identical fundamental frequencyvector pairs; and selecting fundamental frequency vectors for the Nhalftone screens according to (V_(i1),V_(i2))=(m_(i1)V_(R1)+m_(i2)V_(R2), n_(i1)V_(R1)+n_(i2)V_(R2)) forinteger m's and n's, where at least one fundamental frequency vector orits conjugate must also satisfy one of the following: V_(ik)=V_(R1),V_(ik)=V_(R2), and ″V_(ik)|>2 max [|V_(R1)|, |V_(R2)|]. The disclosurefound in U.S. Pat. application 20080130054 is hereby incorporated byreference in its entirety.

A current practice for resizing an image is to perform some type ofresampling interpolation of the input image to generate an output imagewith the desired number of samples in each dimension. But, resampling acolor halftone image with an interpolator such as nearest-neighbor,linear, quadratic, or cubic can result in defects within the colorhalftone image. One particularly problematic defect is the introductionof gray levels that must be re-halftoned prior to printing, where there-halftoning step creates an interference pattern with the input colorhalftone image structure. Another defect is the appearance of seamsalong columns or rows of pixels, where the resampled halftone sampleshave a local disturbance in phase with respect to the halftonefrequency. Yet another defect associated with these resampling methodsis that the aspect ratio of important image content can becomedistorted. For example, use of resampling to reduce the verticaldimension of an image can make people appear shorter and wider than theyare in reality.

Another practice for resizing a color halftone image is simply to cropthat image to the desired size. However, cropping can delete desiredimage content around the borders of the color halftone image.

The diversity and versatility of display devices today imposes newdemands on digital media. For instance, designers must create differentalternatives for web-content and design different layouts for differentdisplay and rendering devices. These demands have lead to development ofincreasingly sophisticated image resizing tools for continuous tonedigital images. Avidan and Shamir, in “Seam Carving for Content-AwareImage Resizing” ACM Transactions on Graphics, Volume 26, Number 3,SIGGRAPH 2007, present a simple image operator called seam carving, thatsupports content-aware image resizing for both image reduction and imageexpansion. A seam is an optimal eight-connected path of pixels on asingle image from top to bottom, or left to right, where optimality isdefined by a low value of an image energy function. By repeatedlycarving out or inserting seams in one direction, Avidan and Shamir canchange the aspect ratio of an image. By applying these operators in bothdirections they can retarget the image to a new size. The selection andorder of seams protect the content of the image, as defined by theenergy function. Seam carving can also be used for image contentenhancement and object removal. The seam carving method of Avidan andShamir can support various visual saliency measures for defining theenergy of an image, and can also include user input to guide theprocess. By storing the order of seams in an image they createmulti-size images that are able to continuously change in real time tofit a given size.

The method of Avidan and Shamir cannot be readily applied to colorhalftone images because selecting low energy seams will result invisually undesirable pathological seams that travel between halftonedots or along chains of connected dots. Removing a low-energy seam thattravels between halftone dots would only increase the local darkness inthe region about the seam. Conversely, removing a low-energy seam thattraveled along connected halftone dots will decrease local darkness inthe region about the seam. In either case, the seams would appear asvisible streaks and would quite likely be objectionable. For example asimple single separation input halftone image where the pixels are at600 dpi (dots per inch) resolution, and the halftone is at 141 cpi(cells per inch) at 45° when resized by 10% in the horizontal directionby applying a low energy seam removal method directly on the halftoneimage caused undesirable streaks to appear in the image.

One further option for resizing a halftone image is to apply adescreening technique to the halftone image to remove the halftone dotstructure and provide a continuous tone version of the image. Thecontinuous tone version of the image could be resized using the methodof Avidan and Shamir. After resizing, the image may be re-halftoned tofinally produce a resized binary image. However, a key problem with thatapproach is that any such descreening technique tends to blur finedetails within an image and the resulting image will have an excessively“soft” appearance. This softness problem will be particularly evidentwhen applied in binary printer image paths and copier image paths thatutilize a “copy dot” approach to reproduction. “Copy dot” refers todirect copying of a halftone image without descreening and rescreening.Resizing such a descreened image will induce a blurring that “copy dot”reproduction is intended to avoid.

As provided herein, there are supplied teachings to systems and methodsfor resizing a digital uniform rosette halftone image composed ofmultiple colorant separations, by using uniform rosette halftone tileparameters. One approach entails receiving into a digital imagingsystem, a digital uniform rosette halftone image and a desired resizingfactor for the digital uniform rosette halftone image. Subsequently thesystem will define uniform rosette cells within the color uniformrosette digital halftone image. From the defined uniform rosette cells,a number of uniform rosette halftone tile seams are determined formanipulation. The orientation of the number of uniform rosette halftonetile seams being dictated by the received desired resizing factor. Anenergy map of the digital uniform rosette halftone image is determinedaccording to an energy metric derived from the multiple colorantseparations. The energy of the number of uniform rosette halftone tileseams within the energy map is determined so as to provide indication ofat least one low energy determined uniform rosette halftone tile seam. Aresizing of the uniform rosette halftone image by manipulating the atleast one low energy determined uniform rosette halftone tile seam isperformed so as to obtain a resized uniform rosette halftone image. Theresized uniform rosette halftone image may then be printed on a printer.

Disclosed in embodiments herein is a method for resizing a digitaluniform rosette halftone image composed of multiple colorantseparations. The method provides receiving into a digital imagingsystem, a digital uniform rosette halftone image and a desired resizingfactor for that digital uniform rosette halftone image. The system willthen determine the uniform rosette halftone screen parameters for thedigital uniform rosette halftone image. Uniform rosette cells within thedigital uniform rosette halftone image from the determined uniformrosette halftone screen parameters are then defined. From the defineduniform rosette cells and determined uniform rosette halftone cellparameters, a number of uniform rosette halftone tile seams aredetermined for manipulation. The orientation of these uniform rosettehalftone tile seams being dictated by the received desired resizingfactor. An energy map of the digital uniform rosette halftone image isdetermined according to an energy metric derived from the multiplecolorant separations. The energy of the number of uniform rosettehalftone tile seams within the energy map is determined so as to provideindication of at least one low energy determined uniform rosettehalftone tile seam. A resizing of the uniform rosette halftone image bymanipulating the number of low energy determined uniform rosettehalftone tile seams is performed to obtain a resized uniform rosettehalftone image. The resized uniform rosette halftone image may then beprinted on a printer.

Further disclosed in embodiments herein is an image forming method forresizing a digital uniform rosette halftone image composed of multiplecolorant separations. The method entails receiving into a digitalimaging system, a digital uniform rosette halftone image and a desiredresizing factor for the digital uniform rosette halftone image. Uniformrosette cells within the digital uniform rosette halftone image aredefined. From the defined uniform rosette cells, a number of uniformrosette halftone tile seams are determined for manipulation. Theorientation of these uniform rosette halftone tile seams being dictatedby the received desired resizing factor. Each colorant separation of thedigital uniform rosette halftone image is descreened to providedescreened pixel values. An energy metric from the descreened pixelvalues is determined so as to provide an energy map. The energy of thenumber of uniform rosette halftone tile seams is determined according toan energy map, so as to indicate of a number of low energy determineduniform rosette halftone tile seams in sufficient number to at least toachieve the desired resizing factor for the digital uniform rosettehalftone image. A resizing of the uniform rosette halftone image isperformed by manipulating the number of low energy determined uniformrosette halftone tile seams, to obtain a uniform rosette resizedhalftone image. The resized uniform rosette halftone image may then beprinted on a printer.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 depicts an exemplary embodiment of a digital imaging systemsuitable for one or more aspects of the present invention.

FIG. 2 Schematic depicting an embodiment of the method taught herein.

FIG. 3 Schematic depicting relationship between pixels, halftone spatialvector representation, and parameters that relate to Holladayrepresentation.

FIG. 4 Schematic depicting relationship between pixels, a rotatedhalftone screen, a Holladay tile, and the parameters in the Holladayrepresentation.

FIG. 5 depicts an example of Holladay halftone tiles and a verticalhalftone tile seam connecting low energy tiles.

FIG. 6 depicts an exemplary cyan halftone pattern and its Fourierrepresentation.

FIG. 7 depicts an exemplary magenta halftone pattern and its Fourierrepresentation.

FIG. 8 depicts an exemplary black halftone pattern and its Fourierrepresentation.

FIG. 9 depicts the superimposition of exemplary cyan, magenta, and blackhalftone patterns, with the corresponding Fourier representation forthat exemplary superimposition along-side.

FIG. 10 depicts the Fourier representation of FIG. 9 with the rosettevectors and halftone fundamental spectral hexagon illustrated.

DETAILED DESCRIPTION

The teachings herein are directed to a method and apparatus for resizinga halftone image using uniform rosette halftone tile parameters. Inparticular, the teachings herein resize an image by manipulating uniformrosette halftone tiles or cells along low energy uniform rosettehalftone tile seams. By using the tile parameters to define the lowenergy uniform rosette halftone tile seams, a uniform rosette colorhalftone image can be resized while avoiding the defects associated withapplying known resizing methods directly to color halftone images.

In one embodiment of the teachings herein, a digital uniform rosettecolor halftone image is received and a region of the digital uniformrosette color halftone image is resized through manipulation (be itreplication or deletion) of low energy uniform rosette halftone tileseams within the color halftone image. Uniform rosette halftone cellparameters are received or derived from analysis of the color halftoneimage. A resizing factor or factors are received and are used todetermine if the manipulation is directed to replicate low energyuniform rosette halftone tile seams or delete low energy uniform rosettehalftone tile seams, and to determine the orientation of the seam to bemanipulated (vertical or horizontal). The resizing factor and the cellparameters are used to determine what number of low energy uniformrosette halftone tile seams need to be removed or duplicated.

The energy of uniform rosette halftone tile seams within the halftoneregion is determined using an energy metric, which is a measure of imageactivity within a local region. That energy metric may be derived on apixel basis and spatially quantized to conform to uniform rosettehalftone tiles, or it may be derived directly from the tiles. The energymetric may also be a function of descreened values of pixels within theuniform rosette halftone image region. This energy metric as determinedfor locations within the uniform rosette halftone image region is usedto form an energy map.

The energy of the uniform rosette halftone tile seams is determined byusing the energy map, where uniform rosette halftone tile seams are aconnected path of cells that run either vertically or horizontallythrough the image region depending on the required resizing. The energyof a uniform rosette halftone tile seam is a function of the integratedenergy along the path of the uniform rosette halftone tile seam. Anumber of low energy uniform rosette halftone tile seams will bemanipulated, where the number depends on the resizing factor and theuniform rosette halftone cell parameters. Resizing factors greater than1 are defined to require low energy uniform rosette halftone tile seamreplication while resizing factors less than 1 require low energyuniform rosette halftone tile seam deletion.

The low energy uniform rosette halftone tile seams are manipulatedaccording to their energy ranking, where uniform rosette halftone tileseams possessing lowest or relatively low energy are selected first formanipulation. A seam is considered a low energy seam if its energy isbelow a threshold, which may be a function of the energy level of theminimum energy seam. Low energy uniform rosette halftone tile seams canbe manipulated either as a group, or the manipulation can be performediteratively, where within the iterations, uniform rosette halftone tileseam energy is recomputed when one or more low energy uniform rosettehalftone tile seams are removed or replicated, and the recomputeduniform rosette halftone tile seam energy is used for ranking andsubsequent manipulation.

For a general understanding of the present invention, reference is madeto the drawings. In the drawings, like reference numerals have been usedthroughout to designate identical elements. In describing the presentinvention, the following term(s) have been used in the description.

The term “cell” indicates consistent unit area and shape of pixels orhalftone threshold values arrayed in manner that fills a region withoutforming gaps. In a monochrome image, for example black and white, or asingle color separation, a cell refers to pixels or threshold valueswithin a single spatial two-dimensional array. In a multi-separationuniform rosette color image (e.g., cyan, magenta, yellow, and black) acell in the present context can refer to pixels or threshold valuesacross the multiple separations.

The terms “tile” and “Holladay tile” are used synonymously within thepresent disclosure, and indicate cells that are rectilinear in shape,constructed of vertical sides and horizontal sides. Due to thesecharacteristics they are convenient for use in horizontal or verticalresizing. In a monochrome image, for example black and white, or asingle color separation, a tile refers to pixels or threshold valueswithin a single spatial two-dimensional array. In a multi-separationcolor image (e.g., cyan, magenta, yellow, and black) a tile in thepresent context can refer to pixels or threshold values across themultiple planes.

There are several equivalent representations for the periodic structureof a halftone image. For example, parameters that describe the tiling ofcells or parameters that describe the tiling of Holladay tiles bothfully describe the halftone structure for an image. Thus, “cellparameters” and “tile parameters” and related representations describedmore fully below possess equivalent information and transformations maybe made between the representations.

The term “uniform rosette” refers to a moiré-free hexagonal structureformed from the overlay of multiple halftone color separations, wherethe period and angle of the hexagonal structure are consistentthroughout an image region. Uniform rosettes color halftones aredescribed in U.S. Pat. No. 6,798,539 to Wang et al. Uniform rosettescolor halftones are also described in U.S. Patent ApplicationPublication No. 2008/0130055 A1 to Wang and Loce, and U.S. PatentApplication Publication No. 2008/0130054 to Wang and Loce. Uniformrosette halftones are also described more full below.

“Descreening” refers to methods to remove the halftone dot structure orhalftone rosette structure of an image to produce a continuous toneversion of the image.

“Eight-connectivity” commonly refers to pixels that touch neighboringpixels either on a side or a corner, where it is understood that anyflat edge of a tile or pixel is considered a side regardless oforientation. That is, if two pixels are adjacent, side-by-side orcorner-touching, they are said to be eight-connected. We extend thedefinition of eight-connectivity of pixels, to cells of pixels to referto a neighboring relationship between two cells where at least one pixelin the first cell is eight-connected to at least one pixel in the secondcell. An “eight-connected path” is an unbroken string of eight-connectedpixels or eight-connected cells.

A “seam” is an optimal eight-connected path of pixels on a given imagefrom top to bottom, or left to right, where optimality is defined by alow value of an image energy function. A “low energy seam” is a seampossessing an energy metric that is below a threshold level. Thethreshold level can be a function of the energy level of the minimumenergy seam, such as 20% greater than the energy level of the minimumenergy seam.

In a monochrome image, “energy” refers to the variation in gray levelsaround a pixel or variation in halftone cell values around a halftonecell. In a uniform rosette halftone image, “energy” refers to thevariation in a color metric around a pixel or variation in uniformrosette halftone cell values around a uniform rosette halftone cell. Thecolor metric can be a measure within a perceptually uniform space, suchas CIE Lab. Neighboring pixels or neighboring cells that have similarvalues possess low energy, while neighboring pixels or neighboring cellsthat possess very different values possess higher energy. An energymetric is a measure of energy, such as the sum of the magnitude of thegradient along an eight-connected path.

Within the field of halftoning, the term “screen” is sometimes used todenote an array of threshold values, and sometimes used to denote theperiodic structure of a halftone image. Within the present disclosure weare not concerned with a halftoning process, so use of the term “screen”herein will denote the periodic halftone structure unless the contextrefers to a screening process.

In FIG. 1, as depicted therein is one embodiment of a digital imagingsystem suitable for one or more aspects of the present invention. In thesystem 110, image source 120 is used to generate image data that issupplied to an image processing system 130 (including a digital frontend), and which produces output data for rendering by print engine 140.Image source 120 may include scanner 122, computer 124, network 126 orany similar or equivalent image input terminal. On the output endprinter engine 140 is preferably a xerographic engine however printengine 140 may include such equivalent print technology alternatives aswax, ink jet, etc. The teachings presented herein are directed towardaspects of image processor 130 depicted in FIG. 1. In particular, theintention of the teachings presented herein is to identify, and renderaccordingly, seams within a digital image. It will be appreciated bythose skilled in the art that the rendering of an image into a printableor displayable output format may be accomplished at any of a number oflocations, which herein is provided for in but one example only asoccurring within the image processing system 130 or within in the printengine 140.

Many applications can be envisioned within the system embodiment 110.For instance, consider that a document can be rasterized and halftonedby a computer 124 for a particular print path and printer 128. Thatdocument may be directed to a different printer 140, possibly yearslater when extracted from an archive 129, with different paper sizecapabilities and may require image editing, cropping and resizing ofhalftoned image content prior to printing on the given print engine.Halftoned images may be acquired from a scanner 120 or retrieved from anarchive 129 as part of a document to be re-purposed. The document may bedirected to print on different paper sizes, and may be redesigned withdifferent layout requirements, thereby requiring resizing of its variouselements, such as the halftone image. Printed halftone images may bescanned using a scanner 122 in a setting such as at a digital copier,and a user may wish to modify the image attributes such as size, aspectratio, or image content prior to printing on a printer 140.

FIG. 2 provides a schematic for embodiments directed to the methodtaught herein. One embodiment of the method receives a uniform rosettecolor halftone image region 310 and a resizing factor or factors. Afactor indicates a desired magnification change for a particularorientation (e.g., vertical or horizontal). The magnification factorcorresponds to a number of rows or columns of pixels to be deleted orreplicated. An alternative to receiving a magnification factor isdirectly receiving the number of rows or columns of pixels to bemanipulated within the region 320. Uniform rosette halftone tileparameters can optionally be input or they can be estimated from theuniform rosette halftone image 330. The method applies a descreeningoperation 340 to the input uniform rosette halftone image to produce acontinuous-tone image. Optionally, the descreened image values can bemapped from a device dependent color space to a perceptually uniformcolor space 345, which allows the energy metric to better correspond toperceived image activity. The descreening operation may use the uniformrosette halftone tile information so that the halftone rosette texturemay be well removed. Seams are found within the contone image 350. Theuniform rosette halftone tile seams are determined from connecteduniform rosette halftone tiles or determined from connected pixels andconverted to connected uniform rosette halftone tiles. The low energyseams of connected tiles (low energy uniform rosette halftone tileseams) are either removed or replicated 360 as needed in the inputuniform rosette halftone image until 370 the desired resizing isachieved and a resulting rescaled uniform rosette halftone image isoutput 380.

Halftone tile parameters may be known in some image processing settings.For instance, in a binary printer image path, the Digital Front End(DFE) 130 of the print engine 140 may possess one or more halftonethreshold arrays that are used to performed the halftoning operation.Knowledge of the halftone threshold arrays can provide the halftone tileinformation. If the halftone tile information is not known a priori, itcan be derived via a frequency analysis. For instance, digital imageprocessing analysis can be used to estimate the halftone cell parametersof a scanned halftone image in a digital copier setting. Varioustechniques have been applied to this estimation problem, such as findingthe maximum of an autocorrelation or Fourier transform, or performingwavelet analysis. Examples of methods for estimating halftone parametersare taught by Schweid in U.S. Pat. No. 6,734,991, Shiau and Lin in U.S.Pat. No. 7,239,430, and Lin and Calarco in U.S. Pat. No. 4,811,115. Thedisclosure found in these patents is hereby incorporated by reference inits entirety.

Key to the present invention is an understanding of halftone periodicstructures, halftoning tiling and halftone tile parameters. We firstdiscuss uniform rosette halftoning, then describe cell representations.

The four plots in FIGS. 6-9 provide examples of uniform rosettehalftones and their respective spatial frequency representations, whichwill be used to teach the concepts of uniform rosette halftoning. Thehalftones are shown on the left and frequency representations on theright. Of course, the halftones possess many higher order harmonics thatare not shown in the plots due to limiting the range of the plots to±300 cycles-per-inch (cpi) in both directions to simplify the plots forteaching the relevant concepts.

Most screening-based halftone methods use halftone screens in atwo-dimensional tiling manner. Thus the corresponding halftone outputspossess strong periodic structures defined by the halftone screens.Images can be also described by their Fourier transforms or theirspatial frequency representations. As the result of tiling halftonescreens, Fourier transforms of the halftone patterns in FIGS. 6-8 aredominated by discrete frequency components defined by the twofundamental halftone frequency vectors for each screen and theirtwo-dimensional higher-order harmonics, or linear combinations of thefundamentals. For the following discussion in this specification, we usethe notation illustrated by the transform plots in FIGS. 6-8 torepresent the Fourier transform of halftone patterns. Only the locationsof the fundamental halftone frequency vectors, V_(c1), V_(c2), V_(m1),V_(m2), V_(k1), and V_(k2), and some of their harmonics are shown in thespatial frequency coordinates as circular dots, and the amplitude andphase of each component are ignored in these illustrations. The sub 1and sub 2 notation refers to vectors that are above (0° to 90°) or below(270° to 360°, or equivalently −90° to 0°) the 0° axis, respectively. Weuse this notation consistently within the present disclosure torepresent the two quadrants. Unless otherwise noted, we use thesubscripts c, m, y, and k, to aid in teaching the presently describedhalftoning processes due to the common practice of four-color printingwith cyan, magenta, yellow, and black. While we teach using thatnotation, the concepts are general in that other colorants may be used.For example, we may use the notation V_(m1) and use examples that referto it as a frequency vector for the magenta screen, but it is to beunderstood that we intend it to generally imply a frequency vector inthe first quadrant for some available colorant. Further, we note thatcolorants for particular screen geometries are interchangeable. Forexample, we may teach with yellow halftoned with a screen of a firstgeometry, and black halftoned with a screen of a second geometry, but itis practical and reasonable to assume that the screens may beinterchanged and yellow may be halftoned with the screen of the secondgeometry and black the first.

In color printing, more frequency components than the fundamentalfrequencies are typically created in the halftone image due to thesuperimposition of halftone screens for different process colors. UsingFourier analysis, we can express the result caused by suchsuperimposition of two different colors as their frequency-vectordifference, e.g., V_(cm)=V_(c)±V_(m), where V_(x) represents any ofV_(x1), −V_(x1), V_(x2), −V_(x2), and V_(cm) is the combined vector. Thesign definition of frequency vectors is rather arbitrary since eachFourier component has its conjugate, i.e., there is always a frequencyvector −V_(c) that represents the conjugate component of V_(c). For eachhalftone dot screen, there are two fundamental frequency vectors, thusthe color mixing of two screens for two different colors yields eightunique combined vectors for the fundamental frequency vectors alone.Without judicious design procedures, one or more combined vectors canoccur at relatively low frequencies and possess an objectionableappearance known as moiré.

The common strategy to avoid objectionable two-color moiré is to selectfrequency vectors that ensure that no two-color difference vector of thefundamental halftone frequency vectors is sufficiently small, or shortin length, to be perceived as a noticeably low frequency. The two-colormoiré-free condition can be summarized by

|V _(c) ±V _(m) |>V _(high),   (1)

where V_(c) represents any one of V_(c1), −V_(c1), V_(c2), −V_(c2);V_(m) represents any one of V_(m1), −V_(m1), V_(m2), −V_(m2); andV_(high) is a frequency limit set at somewhere between 50-70cycles-per-inch for just noticeable moiré.

It is well known that a troublesome moiré is the three-color moiré,which can appear in cyan-magenta-black prints produced by CMYKfour-color printers. As an extension of the two-color case, one aspectof the three-color moiré-free condition can be summarized by

|V _(c) ±V _(m) ±V _(k) |>V _(high),   (2)

where V_(k) represents any one of V_(k1), −V_(k1), V_(k2), −V_(k2); andV_(high) is set similar to the two-color case. Since there arealtogether thirty-two unique combinations of different color componentsfor the left side of the inequality of Equation (2), it stands as amatter of practicality that to make all three-color difference vectorsas well as all two-color difference vectors large enough to avoid anycolor moiré is very difficult, unless the halftone screens have veryhigh frequency fundamentals, say higher than 200 line-per-inch. Anotheraspect of the moiré-free condition is to make two of the three-colordifference vectors null while keeping the rest large. Given that boththe signs and the indices of frequency vectors are defined somewhatarbitrarily, without losing the generality, the three-color moiré-freecondition can be specified by the following vector equation:

V _(c1) −V _(m1) +V _(k2)=0,   (3a)

or, equivalently due to the conventional screen configuration,

V _(c2) −V _(m2) −V _(k1)=0   (3b)

The Equations (3a) and (3b), are two of all possible frequencycombinations of the three colors. In most practical applications, therest of the combinations satisfy the inequality of Equation (2) forV_(high) as large as MIN[|V_(c)|, |V_(m)|, |V_(k)|] and are notspecially specified, and the combination of halftone outputs produce arosette appearance rather than objectionable moiré.

Most conventional halftone screens use square-shape halftone cells fortiling. Therefore, the two fundamental frequency vectors of each screenare not independent to each other. Once one of the two equations, either(3a) or (3b) is satisfied, the other one is automatically held.Recently, Wang et al. has taught halftone methods (U.S. Pat. No.6,798,539, Wang et al. as incorporated by reference above) usingnon-orthogonal halftone cells to construct halftone screens, or generalparallelogram-shape halftone cells, for moiré-free color halftoning, inwhich case the two fundamental frequency vectors of eachparallelogram-shape-based screen are independent to each other and thussatisfying both Equations (3a) and (3b) is required for the three-colormoiré-free condition. We note that the term “non-orthogonal” as used inthe present specification here refers to “not necessarily square,” whichis less restrictive than “strictly not orthogonal.” Such terminologyfollows convention used in mathematics, where terms such as “non-linear”refers to “not necessarily linear.”

Further concerning moiré-free non-orthogonal halftone configurations,Wang, in US Publication No. 2006/0170975 A1, disclosed a moiré-freecolor halftone configuration for clustered dots. Unlike conventionalmethods, the disclosed method produces periodic hexagon rosettes ofidentical shapes. These exemplary hexagon rosettes have threefundamental spatial frequencies exactly equal to half of the fundamentalfrequency of the three halftone screens. The resultant halftone outputsare truly moiré free, as all the fundamentals and harmonic frequenciesare multiples of and thus higher in frequency than the rosettefundamental frequency.

An example of a hexagonal rosette halftone configuration is easy tounderstand through extension of the classical screen configuration.Assume halftone screens rotated to 15°, 45°, and 75°, respectively, forthree different colors. In the present example, the halftones screenswill satisfy Equation (3), but will be constructed of rectangular cells,rather than square cells. The monochromatic halftone outputs of thisconfiguration, shown as C, M and K halftone patterns, and their spectraare shown in FIGS. 6, 7, and 8, respectively. The repeated halftonepattern for each separation of this configuration is a rectangular cellwith a ratio between the lengths of the two sides equal to 0.866, orexactly cos(30°). The frequency representations of the halftone patternsshow that fundamental frequencies vectors of each pattern areperpendicular to each other and the ratio of the two frequencies arealso equal to cos(30°).

In FIG. 9, the superimposition of the C, M, and K halftone patterns ofFIGS. 6, 7 and 8 is shown on the left, and the frequency representationof the superimposition is shown on the right. In the frequencyrepresentation, fundamental frequencies and harmonics of eachmonochromatic screen are illustrated by dots of the color of thatscreen. Gray dots indicate a frequency formed by the interactions ofmultiple screens. We see that the rosette of FIG. 9 has a relativelysimple, uniform appearance, which results in a pleasing texture.

Besides the pleasant appearance of the rosettes, an interestingobservation is that all frequency components, including all fundamentalfrequencies and the respective harmonics of the monochromatic halftones,and frequencies due to all possible color combinations, can be located ahexagonal grid in the Fourier representation. The hexagonal grid can beseen by drawing a line connecting the nearest neighbors of any point inthe spectra.

The halftoning method, and resulting configuration utilized in uniformrosette image resizing method taught herein is based on defining rosettefundamental frequency vectors, of sufficiently high frequency and angleseparation, that can be used to generate a hexagonal lattice of rosetteharmonics. The lattice is generated by linear combinations of therosette fundamental frequency vectors. Angles and frequencies forindividual halftone screens are chosen from the rosette lattice points.A screen set selected in such a manner is moiré free because nocombination of frequency lattice points can produce a beat lower thanthe two rosette frequency vectors used to generate the lattice. Thelattice structure defined by the rosette makes it possible to choosepairs of frequency vectors for an almost arbitrary number of colorantswithout introducing any moiré in an N-color combination. N-colorcombinations occur in printing systems that employ N colorants. Theseprinting systems use colorants sets other than simply the conventionalCMYK set. For instance, N-color printing systems may include colorantssuch as orange, green, violet, red, blue, gray, light cyan, lightmagenta and dark yellow, in addition to the CMYK colorants. N-colorantsystems also refers to printing with a smaller set of colorants, such asblack and one highlight colorant. Practical frequency lattices can berealized through the use of nonorthogonal screens.

To better understand this rosette vector concept, consider the exampleof FIG. 9. Rosette vectors V_(R1), V_(R2) shown as red dashed vectors,and the lowest frequency components of the rosette are shown as circles.Note that is it easy to see that the set of lowest frequency componentsform the vertices of a hexagon. We refer to the hexagon formed by thelowest frequency components as the “first-order spectral hexagon.” Therelationships between the screen frequency vectors and rosette vectorsare given by

V _(c1)=2 V _(R1) −V _(R2)

V_(c2) =2 V _(R2)

V _(m1) =V _(R1) +V _(R2)

V _(m2)=−2 V _(R1)+2 V _(R2)

V_(k1)=2 V_(R1)

V _(k2) =−V _(R1)+2 V _(R2)

The conjugate fundamental frequency vectors are also shown in FIG. 9.The figure shows that the set of all halftone fundamental frequenciescan be connected to form a hexagon, illustrated in FIG. 9 as a thinblack line. The halftone fundamental frequencies form the vertices aswell as define points that roughly bisect the sides of the hexagon. Thishexagon connects the frequency components that lie just outside of the“first-order spectral hexagon. We refer to this hexagon as the“second-order spectral hexagon.”

We now turn to teaching equivalent forms of halftone structurerepresentation, such as frequency vectors, spatial vectors and Holladaytile parameters. Knowing one representation and its parameters allowsdetermination of a form that is most convenient for the halftone tileseam manipulation. Due to the rectilinear characteristics of Holladaytile parameters, they are convenient for use in horizontal or verticalresizing. Due to the equivalence in representing halftone structure,within the present disclosure we often simply write “halftone tileparameters.”

Rationally angled periodic halftone screens can be represented inseveral equivalent forms. For instance, the periodic structure is oftendescribed by either two spatial vectors or two frequency vectorsspecifying the frequency and orientation of halftone periodicity. Forpresenting the teachings herein, a useful representation for halftoneperiodicity is the replication of rectangular cells with vertical andhorizontal sides. For rationally angled periodic screens, Holladay, inU.S. Pat. No. 4,185,304 has shown that there is such a rectangularhalftone cell representation that is equivalent to the spatial vectorand frequency vector representations. The disclosure found in U.S. Pat.No. 4,185,304 is hereby incorporated by reference in its entirety. Therepresentation of the equivalent rectangular cell requires only threeparameters in addition to the threshold values. We use the term“Holladay tile” to denote the tiles associated with halftone tilingutilizing rectangles having vertical and horizontal sides.

FIG. 3 teaches the relationship between halftone vector representation,which is often used to represent halftone cells aligned on a rationalangle, and rectangular tile representation. Let z₁ 410 be the spatialvector located in the first quadrant and let z₂ 420 be the frequencyvector located in the fourth quadrant. The halftone screen representedby the spatial vectors z₁ and z₂ can be thought of as the replicationsof parallelogram halftone cells with sides of length ∥z₁∥ and ∥z₂∥ atangles ∠z₁ 430 and ∠z₂ 440, where ∥z∥ is the norm of vector z and ∠z isits angle. Let z_(i)=(x_(i),y_(i)) be the rectangular coordinaterepresentation of the vector whose polar coordinate representation is(∥z_(i)∥,∠z_(i)), for i=1, 2. For a rationally angled halftone screen,x_(i) and y_(i) are integers. The area of each parallelogram is

A=∥(x ₁ , y ₁)×(x ₂ , y ₂)∥=x ₂ y ₁ −x ₁ y ₂,   (1)

where × is the vector cross-product operator.

Alternatively, frequency vectors f₁ and f₂ may be provided instead ofspatial vectors when specifying the halftone screen. Vector f_(i) isparallel to vector h_(i), which is the height of the parallelogramperpendicular to vector z_(i) for i=1, 2 as illustrated in FIG. 4. Themagnitude of vector f_(i) is equal to the reciprocal of the magnitude ofvector h_(i) for i=1, 2.

Let L be the shortest distance along the horizontal axis in which theparallelogram pattern recurs (points 3 450 and 4 460 in FIG. 4), and letL 470 be its corresponding vector. Since L 470 is obtained by followinga path along the sides of the parallelogram, it must be the result ofthe addition of an integer number of vectors z₁ 410 and z₂ 420.Mathematically,

L=k z ₁ +j z ₂,   (2)

where k and j are the smallest integer values that satisfy the equation.Decomposing Eq. (2) into its components, we get

L=k x ₁ +j x ₂,   (3)

0=k y ₁ +j y ₂.   (4)

Let p be the greatest common divisor of y₁ and y₂. Then

p=−y ₁ /j=y ₂ /k≧1.   (5)

Combining Eq. (5) with Eq. (3) and substituting into Eq. (1) gives area

A=Lp.   (6)

Since A and p are known (either z₁ 410 and z₂ 420 or f₁ and f₂ areknown), L can be calculated.

A similar analysis in the vertical direction yields area

A=Kq,   (7)

where K is the shortest vertical distance in which the parallelogrampattern recurs and q is the greatest common divisor of x₁ and x₂. SinceA and q are known, K can be calculated.

Equations (6) and (7) imply that an integer number of trapezoids witharea A fit inside a rectangle with dimensions K height and L width. Thisis an insight into the equivalence between halftone screenrepresentation using rationally-angled trapezoids and representationusing Holladay tiles.

Equation (6) implies that the area of one parallelogram is contained ina rectangular block of area A=Lp (see FIG. 4), which must repeat itselfa distance of p 510 units in the vertical direction but displaced in thehorizontal direction a certain amount D 520 to account for the slant ofthe original halftone screen so that it falls on the same position inthe angled grid defined by the screen (see points 1 and 3 in FIG. 4). Inorder to get from point 1 480 to point 3 450, a path defined by thevectors D 490 and p 495 may be followed; alternatively, a path obtainedby concatenating an integer number of vectors z₁ 410 and z₂ 420 can alsobe traced. In mathematical terms,

D+p=m z ₁ +n z ₂,   (8)

which has a unique solution for D 490, m and n if additional constraintssuch as m≧n and D≦L are imposed. Successive displacements by D 520 inthe horizontal direction and p 510 in the vertical direction give thelocation for the next rectangular cell of horizontal width L 530 witharea A. This means that, in effect, a rectangular tile and displacementcan represent a rationally-angled screen. The parameters that are neededto uniquely specify a halftone screen using rectangular tiles are L 530,p 510 and D 520.

It should be noted that the above analysis defined a rectangular tilingwith a row-to-row displacement in the horizontal direction. As will beappreciated by those skilled in the art it is straightforward to rotatethe analysis by 90 degrees to define rectangular tiling with acolumn-to-column displacement in the vertical direction.

Further, we must note that tiles that directly correspond to halftonefrequency vectors can be combined to form larger tiles that fill theimage plane. For instance, a halftone defined by a frequency vector of212 cells/inch at 45° constructed from pixels at 600 per inchcorresponds to a Holladay halftone tile that is 2 pixels in height, 4pixels in width, and offset in successive rows by 2 pixels. Those tilescan be groups in many ways to form larger tiles, sometimes referred toas supercells, or multi-centered cells, that cover the image. Oneexample is that two tiles in a row can be combined to form a dual-dottile that is 2 pixels by 8 pixels in dimension, and successive rows areoffset by 2 pixel. An alternative dual-dot tile can be constructed oftiles on two rows to be 4 pixels by 4 pixels in dimension with an offsetof 0 pixels. Those skilled in the art of halftone design can producemany alternative tilings by combining smaller tiles in variations. Withrespect to the teachings herein, resizing using the smallest possibletile is expected to yield the best image quality due to the fineness ofthe tile. On the other hand, a tile composed of multiple smaller tilesoffers the advantage of reduced computation because a larger number ofpixels are affected in each seam manipulation.

The present teachings on equivalent halftone screen representationindicate that a periodic image structure can be represented byrectilinear halftone tiles. Key to the present teaching is theutilization of this representation for uniform rosettes. Uniform rosetteimage structure, as taught above and in the given references, has beendescribed by pairs of frequency vectors. Hence, a uniform rosettehalftone screen configuration also possesses an equivalent tilerepresentation, which can be utilized in resizing color halftone imagesformed of uniform rosettes.

A descreening step is utilized in one embodiment of the teachings hereinto prevent the confounding of the “energy metric” that is used to findlow energy halftone tile seams in the image. Content-aware halftoneimage resizing finds low energy uniform rosette halftone tile seams thatcan be removed or replicated without drastically changing the appearanceof the image, thus producing a graceful resizing of the original image.Descreening produces a continuous-tone (color gray-scale) representationof the input halftone image region and can prevent the presence ofhalftone texture from interfering with the energy metric. Failure toprevent such texture interference could lead to potentially erroneousdecisions as to which regions of the image have the least visible impacton the overall appearance. There are numerous descreening methods thatcan be utilized by one skilled in the art to obtain a continuous-tonerepresentation of the input halftone image. Examples of methods fordescreening are provided in Harrington in U.S. Pat. No. 6,864,994, Fanet al., in U.S. Pat. No. 6,839,152, and De Queiroz et al., in U.S. Pat.No. 5,799,112. The disclosure found in these patents is herebyincorporated by reference in its entirety for their teachings.

Within the present teachings, there are alternative descreeningconfigurations that can be utilized to suppress the uniform rosettehalftone texture. In one embodiment, each color separation can bedescreened using a descreening filter or method optimized for thehalftone frequency vectors of that color separation. This method can bewell suited for orthographic images, where color mixing between colorantseparations has not occurred. Alternatively, the descreening method canutilize a filter or method optimized for the halftone frequency vectorsof the uniform rosette. This method can be used for orthographic images,but may have increased value in a setting where color mixing betweencolorant separations has occurred, as in a scan of a hardcopy halftoneimage.

The color content of an image could be received as a set ofprinter-dependent colorant separations, or as a scan in ascanner-dependent color space. In either case, a mapping from adevice-dependent color space to a perceptually uniform color space suchas CIE Lab which allows the energy metric to better correspond toperceived image activity. This mapping may be achieved in one of manyalternative ways. When the ICC profile information is embedded in theimage, the information included in the look-up table that definesprofile is used to perform the mapping. When the ICC profile informationis missing, and the device is available for characterization, a look-uptable can be constructed that performs the mapping. In the case of aprinter, the look-up table is constructed by printing patches withdifferent colorant combinations and measuring their Lab values with aspectrophotometer or a calorimeter. This defines a transformation fromthe printer-dependent color space to CIE Lab at the nodes of thecolorant combinations when printing the patches. In the case of havingreceived a scanned image, a test page containing patches with known CIELab values is scanned and the corresponding scanner output colors aremeasured. This defines a transformation from the scanner-dependent colorspace to CIE Lab at the nodes of the colorant combinations used to formthe patches. In either case, for colors in between the look-up tablenodes, interpolation techniques may be used to determine thetransformation. When the ICC profile information is missing, and thedevice is unavailable for characterization, conventional formulas fortransformation between color spaces may be used as an approximation.

Alternatively, we may directly convert the pixel values within a givenuniform rosette halftone tile to perceptually uniform values for thattile. This may be accomplished using area-based models for estimatingspectral content of combinations of primaries. An example of such amodel is the well known Nuegebauer equations.

A seam is defined as a low energy eight-connected path that traversesthe image from top to bottom or from left to right. Eight-connectivitycommonly refers to pixels that touch neighboring pixels either on a sideor a corner, where it is understood that any flat edge of a tile orpixel is considered a side regardless of orientation. That is, if twopixels are adjacent, either as side-by-side or corner-touching, they aresaid to be eight-connected. We herein extend the definition ofeight-connectivity of pixels, to uniform rosette cells of pixels torefer to a neighboring relationship between two uniform rosette cellswhere at least one pixel in the first uniform rosette cell iseight-connected to at least one pixel in the second uniform rosettecell. An eight-connected path is defined as an unbroken string ofeight-connected pixels or eight-connected uniform rosette cells. A givenseam as defined for the purposes of the present disclosure can only haveone type of strong connectivity, vertical or horizontal, where strongconnectivity refers to side-to-side touching, as opposed to cornertouching, which is referred to as weak connectivity. For instance, aseam that traverses an image region from top to bottom may not possessstrong horizontal connectivity, and vice versa. Within the teachingsprovided herein, where the distinction between a seam of pixels and aseam of uniform rosette halftone tiles is important, we refer to a seamconstructed of uniform rosette halftone tiles as a “uniform rosettehalftone tile seam.”

FIG. 5 illustrates a low energy uniform rosette halftone tile seamrunning vertically through a section of a digital image. The uniformrosette tiles are formed of 4×8 pixel blocks, where each successive rowof blocks is offset by 4 pixels. In the figure, the darkness of a tilerepresents the energy of that tile. For example, tile 610 is relativelydark and is illustrative of a high energy tile, while tile 620 isrelatively light and illustrative of a low energy tile. A vertical lowenergy halftone tile seam 630 is formed by connecting the centers of lowenergy uniform rosette halftone tiles along a path from the top of theimage section to the bottom of the section. Removing or replicatinguniform rosette halftone tiles along this path 630 would have the leastnoticeable impact on the visual appearance of the image, and thus isdesirable for manipulation for resizing.

The optimality of a seam depends on the desired application. In resizingimages according to the teachings herein, a desired image size isachieved by repeatedly removing or replicating low energy uniformrosette halftone tile seams that run in the appropriate direction. Inthis application, the optimality of a uniform rosette halftone tile seamrefers to the degree to which it would not be noticed upon removal orreplication. In this case, a uniform rosette halftone tile seam isoptimal if the pixels or cells that make up the uniform rosette halftonetile seam are located in regions with little activity as measured by anenergy metric. By activity, we mean variations in color within a spatialregion. A region with high color variation is said to have high activityand would possess a high value energy metric. For continuous tone,monochromatic images, a commonly used energy metric is the imagegradient.

A monochromatic image can be seen as a function of two variables, f(x,y)whose value at (x,y)=(x₀,y₀) is the gray value of the pixel located inrow x₀ and column y₀ of the image. In one embodiment of the presentteachings herein, the energy metric at each pixel is determined as themagnitude of the local image gradient: the larger the local gradient,the larger the energy at that particular pixel. The gradient of atwo-variable function is defined as the two-dimensional vector

$\begin{matrix}{{{\bullet \left( {x,y} \right)} = \left\lbrack {\frac{\bullet \; f\; \overset{'}{Y}}{\bullet \; x\; \overset{'}{Y}}\frac{\bullet \; f\; \overset{'}{Y}}{\bullet \; y\; \overset{'}{Y}}} \right\rbrack},} & (9)\end{matrix}$

with magnitude

$\begin{matrix}{{{{\bullet \left( {x,y} \right)}} = \sqrt{\left( \frac{\bullet \; f\; \overset{'}{Y}}{\bullet \; x\; \overset{'}{Y}} \right)^{2} + \left( \frac{\bullet \; f\; \overset{'}{Y}}{\bullet \; y\; \overset{'}{Y}} \right)^{2}}},} & (10)\end{matrix}$

where ∂fl∂x and ∂fl∂y are directional derivatives in the x and ydirection, respectively. Directional derivatives can be approximated byapplying spatial kernels that compute finite differences. Examples ofsuch spatial kernels are the Prewitt, which are described in“Fundamentals of Digital Image Processing” by A. Jain, Prentice Hall.1989:

$\begin{matrix}{\begin{bmatrix}{- 1} & 0 & 1 \\{- 1} & 0 & 1 \\{- 1} & 0 & 1\end{bmatrix},\begin{bmatrix}{- 1} & {- 1} & {- 1} \\0 & 0 & 0 \\1 & 1 & 1\end{bmatrix},} & (11)\end{matrix}$

and the Sobel, which are described in “Digital Image Processing,” by R.Gonzalez and P. Wintz, Addison-Wesley Publishing Company, 2^(nd)Edition, 1987:

$\begin{matrix}{\begin{bmatrix}{- 1} & 0 & 1 \\{- 2} & 0 & 2 \\{- 1} & 0 & 1\end{bmatrix},{\begin{bmatrix}{- 1} & {- 2} & {- 1} \\0 & 0 & 0 \\1 & 2 & 1\end{bmatrix}.}} & (12)\end{matrix}$

The Laplacian, also described in the books by Jain, and Gonzalez andWintz, is another measure of local energy that is less computationallyexpensive since it only requires the application of one kernel.Mathematically, it is defined as

$\begin{matrix}{{{\bullet^{2}\left( {x,y} \right)} = {\frac{\bullet^{2}}{\bullet \; x} + \frac{\bullet^{2}}{\bullet \; y}}},} & (13)\end{matrix}$

and can be approximated with the kernel

$\begin{matrix}{\begin{bmatrix}0 & 1 & 0 \\1 & {- 4} & 1 \\0 & 1 & 0\end{bmatrix}.} & (14)\end{matrix}$

However, due to the second-order derivative, the Laplacian operator ismore sensitive to noise than the gradient operators.

The gradient-based metric should be applied to halftone images that havebeen de-screened, as direct calculation of the image gradient onhalftone images may yield misleading results that depend on the halftonestructure as well as on the image activity. In one embodiment of theteachings herein, we generalize the concept of the image gradient tohalftone color images by mapping the continuous tone image (obtained byapplying a de-screening filter to the color image) from device-dependentspaces such as RGB or CMYK to a perceptually uniform space such as CIELab and computing the gradient on each color plane separately. The pixelenergy can then be approximated by either the local gradient in theluminance plane only, as it is the most perceptually relevant of thethree, or by merging the energy in each of the three planes via avectorial norm such as the L₂ norm. Other more elaborate alternativesfor calculating the pixel color gradient such as the weighted gradientthat compute the gradient based on the distance of the colors inside agiven connected region, or metrics based on tensorial algebra that usetensors to represent colors in an image and calculate gradients bycalculating the dissimilarity among the tensors may also be used. Anexample of gradients within color images can be found in the publicationby Rittner, Flores, and Lotufo, entitled “New Tensorial Representationof Color Images: Tensorial Morphological Gradient Applied to Color ImageSegmentation,” SIBGRAPI 2007, XX Brazilian Symposium on ComputerGraphics and Image Processing, 2007, pages 45-52.

The energy metrics used for determining low energy seams discussed thusfar have been derived from a contone image representation of thereceived uniform rosette halftone image. It is within the scope of theteachings herein to alternatively derive energy metrics and low energyuniform rosette halftone tile seams directly from the uniform rosettehalftone image. For instance, a measure of rosette-to-rosette differenceis an energy metric. A useful rosette-to-rosette difference metric is acount of the number of pixels within a rosette that are of a differentstate than corresponding pixels within its neighboring rosettes. Statedmathematically,

${E = {\sum\limits_{l}{\sum\limits_{k}{\sum\limits_{i,j}{\left( {C_{l}\left( {i,j} \right)} \right){{XOR}\left( {N_{kl}\left( {i,j} \right)} \right)}}}}}},$

where E is the energy of the rosette C, C_(l)(i, j) are the halftonepixel values of the rosette at positions i, j within colorant separationl, and N_(kl)(i, j) are the halftone pixel values of the rosette atcorresponding positions i, j within the colorant separation l of the kthneighboring rosette, and XOR is the Exclusive OR operation.

Note that other contone energy metrics may be used within the presentteachings, for example functions of the gradient, entropy, visualsaliency, eye-gaze movement, Harris corners, output of face detectors,and other specific feature detectors as discussed by Avidan and Shamirin “Seam Carving for Content-Aware Image Resizing” ACM Transactions onGraphics, Volume 26, Number 3, SIGGRAPH 2007.

One method to determine an optimal seam from energy metrics, is toemploy an exhaustive search that calculates the energy of every possibleseam that originates at each pixel or cell of the first row (column) ofthe image. A more computationally efficient alternative approach is touse a dynamic programming method, because it can eliminate redundancywithin the exhaustive approach. This redundancy is present because seamsoriginating at neighboring pixels (or cells) may have multiple pixels(or cells) in common. Dynamic programming is well known in the field ofcomputer algorithm design.

At each iteration, the dynamic programming approach traverses the energymap row by row to define vertical seams or column by column to definehorizontal seams and finds the cumulative minimum energy at each pixelor cell of each row (or column). At the end of the process fordetermining vertical seams, the smallest value on the last row indicatesthe end point of the optimal path that traverses the image from top tobottom. At the end of the process for determining horizontal seams, thesmallest value on the last column indicates the end point of the optimalpath that traverses the image from left to right. The remaining pixels(or cells) that belong to the seam are found by traversing the energymap in the opposite direction and picking the neighboring pixel (orcell) with the smallest cumulative energy in each subsequent adjacentrow for vertical seams or column for horizontal seams.

Once a low energy halftone tile seam is found, it will need to bereplicated or removed as depending on the resizing factor. To achieveacceptable visual appearance a uniform rosette halftone tile seam doesnot need to possess the absolute lowest energy to be selected forreplication or deletion. It is sufficient for the uniform halftone tileseam to possess relatively low energy as can be determined via an energythreshold. For example, uniform rosette halftone tile seams possessingenergy below a threshold of 5% above the minimum seam energy asdetermined from the image can be selected for manipulation.

As previously noted, replicating or removing a single arbitrary pixel ina row or in a column of a uniform rosette halftone image will introduceresizing streaks. In order to avoid the introduction of artifacts, thepresently taught method manipulates low energy seams constructed ofcells, rather than pixels. Resizing factors greater than 1 require lowenergy uniform rosette halftone tile seam replication while resizingfactors less than 1 require low energy uniform rosette halftone tileseam deletion. A resizing factor that does not equal 1 in the verticaldirection requires manipulation of horizontal low energy uniform rosettehalftone tile seams, while a resizing factor that does not equal 1 inthe horizontal direction requires manipulation of vertical low energyuniform rosette halftone tile seams. Resizing factors not equal to 1 maybe provided for each orientation, and low energy uniform rosettehalftone tile seam manipulation could proceed in serial, one orientationafter the other, or low energy uniform rosette halftone tile seammanipulation could alternate between directions until the adequatenumber of low energy uniform rosette halftone tile seams is manipulatedfor each orientation.

Let the height of the halftone cell be p pixels and its width L pixels.Then at each iteration of low energy uniform rosette halftone tile seammanipulation for a resizing factor less than 1, the removal of a lowenergy uniform rosette halftone tile seam results in the removal of ppixels for vertical manipulation and L for horizontal manipulation.Similarly, at each iteration of low energy uniform rosette halftone tileseam manipulation for a resizing factor greater than 1, the replicationof a low energy uniform rosette halftone tile seam results in thereplication of p pixels for vertical manipulation and L for horizontalmanipulation. Thus, the image is decreased or increased in height orwidth by multiple pixels in each iteration. This implies that if it isdesired to decrease or increase the height or width of the image by mpixels, the process needs to be iterated [m/p] times for verticalmanipulation and [m/L] times for horizontal manipulation, where [·]denotes the rounding operator, which approximates to the nearestinteger. Alternatively, other rounding approaches, such as the nearestlower integer or nearest higher integer may be also be used. Thus, lowenergy uniform rosette halftone tile seam removal can achieve thedesired resizing to the accuracy of the dimensions of a tile since atile is the unit of manipulation.

As we have noted, typically, multiple low energy uniform rosettehalftone tile seams must be manipulated to achieve the desired resizing.There are several alternatives within the scope of the present teachingfor removing multiple low energy uniform rosette halftone tile seams.The alternatives exist because removing one or more seams can affect theenergy metrics of other seams. The alternatives are important becausesome offer the advantage of a lower burden of computation, while otheralternatives may provide better image quality, and yet otheralternatives are a compromise between computational burden and optimalimage quality.

A method for selecting multiple low energy seams that has a lowcomputational burden employs a one-time calculation of seam energy. Thatis, the energy for many uniform rosette halftone tile seams may becalculated one time, and the appropriate number of low energy uniformrosette halftone tile seams can be selected from uniform rosettehalftone tile seams possessing lowest values using the energy of theseams determined from the one-time calculation. When removing multipleseams based on a one-time energy calculation, it must be noted that auniform rosette halftone tile can be a member of one or more seams. Whenthis situation occurs, the seam is manipulated that possesses the lowestenergy. The other seams that contain this tile are then not manipulated.

In terms of perceived image quality, a very high quality resizingproduces an output that introduces the least abrupt density variationdue to seam removal. A method for selecting multiple low energy seamsthat has the potential for achieving the highest image qualityrecalculates seam energy after each manipulation of a low energy uniformrosette halftone tile seam. This method ensures that the absolute lowestenergy seam may be removed. Additionally, the issue of a tile belongingto two or more seams having low energy does not occur.

Alternative methods for removing multiple seams are a compromise betweencomputational burden and optimal image quality. One of these compromisemethods recalculates seam energy after a fixed number of low energyuniform rosette halftone tile seams have been manipulated. Anothercompromise approach to recalculating seam energy is to recalculate theenergy when the next lowest energy uniform rosette halftone tile seamthat has not been removed is sufficiently different in energy from lowenergy uniform rosette halftone tile seams previously removed. There areseveral ways that the difference can be determined. One methodcalculates the difference in energy with respect to the lowest energyseam found in the most recent seam energy calculation. Another methoddetermines difference with respect to the highest energy seam removedthus far. Other differences may also be useful to consider, such asdifference with respect to the mean energy of seam removed thus far.Differences on the order of, say 5% or great may merit an energyrecalculation.

There are also several alternatives within the scope of the presentteaching for replicating multiple low energy uniform rosette halftonetile seams. For example, one low energy uniform rosette halftone tileseam possessing the lowest or relatively low energy (for example, within5% of the minimum energy seam) could be replicated until the resizing isachieved. For some image types it could be desirable to choose lowenergy uniform rosette halftone tile seams for replication that arespatially separated so that a noticeable band of low energy is notinserted into the image. In this situation, some number of spatiallyseparated low energy uniform rosette halftone tile seams could bereplicated to achieve the desired resizing. For example, it can bedesirable to replicate low energy uniform rosette halftone tile seamsthat are separated by 3 or more uniform rosette halftone tiles.

The claims, as originally presented and as they may be amended,encompass variations, alternatives, modifications, improvements,equivalents, and substantial equivalents of the embodiments andteachings disclosed herein, including those that are presentlyunforeseen or unappreciated, and that, for example, may arise fromapplicants/patentees and others.

1. A method for resizing a digital uniform rosette halftone imagecomposed of multiple colorant separations, the method comprising:receiving into a digital imaging system, a digital uniform rosettehalftone image and a desired resizing factor for the digital uniformrosette halftone image; defining uniform rosette cells within the color,uniform rosette digital halftone image; determining from the defineduniform rosette cells, a number of uniform rosette halftone tile seamsto manipulate, where the orientation of the number of uniform rosettehalftone tile seams is dictated by the received desired resizing factor;determining an energy map of the digital uniform rosette halftone imageaccording to an energy metric derived from the multiple colorantseparations; determining the energy of the number of uniform rosettehalftone tile seams within the energy map so as to provide indication ofat least one low energy determined uniform rosette halftone tile seam;performing a resizing of the uniform rosette halftone image bymanipulating the at least one low energy determined uniform rosettehalftone tile seam, to obtain a resized uniform rosette halftone image;and, printing the resized uniform rosette halftone image on a printer.2. The method of claim 1 wherein the multiple colorant separations are aset taken from the group cyan, magenta yellow, black, red, green, blue,violet, gray, light magenta, light cyan, and dark yellow.
 3. The methodof claim 2 where the methodology is only applied to a sub-region of thedigital uniform rosette halftone image.
 4. The method of claim 2 wherethe at least one low energy determined uniform rosette halftone tileseam possesses energy below an energy threshold.
 5. The method of claim4 where the energy threshold is 5% greater than the lowest energydetermined for any of the number of uniform rosette halftone tile seams.6. The method of claim 4 wherein the manipulating of at least one lowenergy determined uniform rosette halftone tile seam is a replicationoperation for increasing the size of the digital uniform rosettehalftone image.
 7. The method of claim 4 wherein the manipulating of theat least one low energy determined uniform rosette halftone tile seam isa deletion operation for decreasing the size of the digital uniformrosette halftone image.
 8. The method of claim 6 wherein themanipulating of the at least one low energy determined uniform rosettehalftone tile seam is a replication operation for a resizing factorgreater than
 1. 9. The method of claim 7 wherein the manipulating of theat least one low energy determined uniform rosette halftone tile seam isa deletion operation for a resizing factor less than
 1. 10. The methodof claim 4 wherein a number of low energy uniform rosette halftone tileseams are manipulated such that this number results in the resizeduniform rosette halftone image possessing the size dictated by theresizing factor within a multiple of the dimensions of a uniform rosettehalftone tile.
 11. The method of claim 4 wherein defining the uniformrosette halftone cells utilizes uniform rosette halftone screenparameters and the parameters are derived from one of autocorrelation,frequency analysis, wavelet decomposition, or directly receiving thescreen parameters.
 12. The method of claim 11 wherein the halftonescreen parameters defining uniform rosette halftone cells are used toderive a Holladay tile representation of the uniform rosette cellscomprising a width, height and offset for the uniform rosette cells, andthe number of low energy uniform rosette halftone tile seams areconstructed of Holladay uniform rosette halftone tiles.
 13. The methodof claim 4 wherein the energy map is derived from one of: colorgradients in each plane in a color space, and calculating thedissimilarity among tensorial representations of colors.
 14. The methodof claim 13 wherein the uniform rosette halftone tile seam is determinedby calculating a low energy pixel seam and quantizing the pixel seam toa uniform rosette halftone tile seam within the energy map.
 15. Themethod of claim 13 wherein the energy map is calculated on a uniformrosette tile basis.
 16. The method of claim 4 wherein the energy map isdetermined on a uniform rosette tile basis by directly calculatingtile-to-tile differences and the difference is summed across the colorplanes.
 17. The method of claim 4 wherein the energy map is determinedon a uniform rosette tile basis by estimating the difference of spectralcontent of the primary colorant combination of each uniform rosettetile.
 18. The method of claim 4 wherein the energy of a uniform rosettehalftone tile seam within the energy map is determined by integratingthe energy of eight-connected cells along the seam that traverses theimage in the direction dictated by the resizing factor.
 19. The methodof claim 8 wherein the resizing factor is greater than 1, therebyrequiring a replication of low energy seams, and one low energy uniformrosette halftone tile seam possessing relatively low energy isreplicated until the resizing is achieved, where low energy is definedto be seam energy within 5% of the minimum energy seam.
 20. The methodof claim 9 wherein the resizing factor is greater than 1, therebyrequiring a replication of low energy seams, and low energy uniformrosette halftone tile seams that are separated by at least the width ofthree tiles are replicated until the resizing is achieved, where lowenergy is defined to be seam energy within 5% of the minimum energyseam.
 21. The method of claim 4, wherein determining the energy of thenumber of uniform rosette halftone tile seams according to an energymetric is one of employing an exhaustive search and employing a dynamicprogramming method.
 22. A method for resizing a digital uniform rosettehalftone image composed of multiple colorant separations, the methodcomprising: receiving into a digital imaging system, a digital uniformrosette halftone image and a desired resizing factor for the digitaluniform rosette halftone image; determining uniform rosette halftonescreen parameters for the digital uniform rosette halftone image;defining uniform rosette cells within the digital uniform rosettehalftone image from the determined uniform rosette halftone screenparameters; determining from the defined uniform rosette cells anddetermined uniform rosette halftone cell parameters, a number of uniformrosette halftone tile seams to manipulate, where the orientation of thenumber of uniform rosette halftone tile seams is dictated by thereceived desired resizing factor; determining an energy map of thedigital uniform rosette halftone image according to an energy metricderived from the multiple colorant separations; determining the energyof the number of uniform rosette halftone tile seams within the energymap so as to provide indication of at least one low energy determineduniform rosette halftone tile seam; performing a resizing of the uniformrosette halftone image by manipulating the number of low energydetermined uniform rosette halftone tile seams, to obtain a resizeduniform rosette halftone image; and, printing the resized uniformrosette halftone image on a printer.
 23. The method of claim 22 whereinthe multiple colorant separations are taken from the group cyan, magentayellow, black, red, green, blue, violet, gray, light magenta, lightcyan, and dark yellow.
 24. The method of claim 22 further comprising thesteps of: descreening the digital halftone image to provide descreenedpixel values; and determining the energy metric from the descreenedpixel values.
 25. The method of claim 22 where the methodology is onlyapplied to a sub-region of the digital uniform rosette halftone image.26. The method of claim 22 where the number of low energy determineduniform rosette halftone tile seams are uniform rosette halftone tileseams that possesses energy below an energy threshold.
 27. The method ofclaim 22 where the energy metric determined for locations within theuniform rosette halftone image forms an energy map.
 28. The method ofclaim 26 where the energy threshold is 5% greater than the lowest energydetermined for any of the number of uniform rosette halftone tile seams.29. The method of claim 26 wherein the manipulating of at least one lowenergy determined uniform rosette halftone tile seam is a replicationoperation for increasing the size of the digital uniform rosettehalftone image.
 30. The method of claim 26 wherein the manipulating ofat least one low energy determined uniform rosette halftone tile seam isa deletion operation for decreasing the size of the digital uniformrosette halftone image.
 31. The method of claim 26 wherein a number oflow energy uniform rosette halftone tile seams are manipulated such thatthis number results in the resized uniform rosette halftone imagepossessing the size dictated by the resizing factor within a multiple ofthe dimensions of a uniform rosette halftone tile.
 32. The method ofclaim 26 wherein the halftone screen parameters defining uniform rosettehalftone cells are used to derive a Holladay tile representation of theuniform rosette cells comprising a width, height and offset for theuniform rosette cells, and the number of low energy uniform rosettehalftone tile seams are constructed of Holladay uniform rosette halftonetiles.
 33. The method of claim 26 wherein the energy map is derived fromone of: color gradients in each plane in a color space, and calculatingthe dissimilarity among tensorial representations of colors.
 34. Themethod of claim 33 wherein the uniform rosette halftone tile seam isdetermined by calculating a low energy pixel seam and quantizing thepixel seam to a uniform rosette halftone tile seam within the energymap.
 35. The method of claim 33 wherein the energy map is calculated ona uniform rosette tile basis.
 36. The method of claim 23 wherein theenergy map is determined on a uniform rosette tile basis by directlycalculating tile-to-tile differences and the difference is summed acrossthe color planes.
 37. The method of claim 25 wherein the energy map isdetermined on a uniform rosette tile basis by estimating the differenceof spectral content of the primary colorant combination of each uniformrosette tile.
 38. The method of claim 27 wherein the energy of a uniformrosette halftone tile seam within the energy map is determined byintegrating the energy of eight-connected uniform rosette cells alongthe seam that traverses the image in the direction dictated by theresizing factor.
 39. A method for resizing a digital uniform rosettehalftone image composed of multiple colorant separations, the methodcomprising: receiving into a digital imaging system, a digital uniformrosette halftone image and a desired resizing factor for the digitaluniform rosette halftone image; defining uniform rosette cells withinthe digital uniform rosette halftone image; determining from the defineduniform rosette cells, a number of uniform rosette halftone tile seamsto manipulate, where the orientation of the number of uniform rosettehalftone tile seams is dictated by the received desired resizing factor;descreening each colorant separation of the digital uniform rosettehalftone image to provide descreened pixel values; determining an energymetric from the descreened pixel values to provide an energy map;determining the energy of the number of uniform rosette halftone tileseams according to an energy map so as to indicate of a number of lowenergy determined uniform rosette halftone tile seams, the number atleast sufficient to achieve the desired resizing factor for the digitaluniform rosette halftone image; performing a resizing of the uniformrosette halftone image by manipulating the number of low energydetermined uniform rosette halftone tile seams, to obtain a uniformrosette resized halftone image; and, printing the resized uniformrosette halftone image on a printer.
 40. The method of claim 39 wherethe methodology is only applied to a sub-region of the digital uniformrosette halftone image.
 41. The method of claim 39 where the energymetric is based on the gradient of luminance.
 42. The method of claim 39where the number of low energy determined uniform rosette halftone tileseams are uniform rosette halftone tile seams that possess energy belowan energy threshold.
 43. The method of claim 42 where the energythreshold is 5% greater than the lowest energy determined for any of thenumber of uniform rosette halftone tile seams.
 44. The method of claim42 wherein the manipulating of at least one low energy determinedhalftone tile seam is a replication operation for increasing the size ofthe digital uniform rosette halftone image.
 45. The method of claim 42wherein the manipulating of at least one low energy determined uniformrosette halftone tile seam is a deletion operation for decreasing thesize of the digital uniform rosette halftone image.
 46. The method ofclaim 39, wherein the received uniform rosette halftone image is one of:orthographic and a scan of a hardcopy halftone image.